Study Notes on Newton's Second Law and Atwood Machine Application
Introduction to Newton's Second Law
Application of Newton's Second Law to systems of objects, such as the Atwood machine.
Instructor: Kristin Gonzalez Vega, Centennial High School, Frisco, Texas.
Example Scenario
Two objects (blocks) with masses denoted as M1 and M2 connected by a string which is pulled by an external force, F0, to the right.
Problem Setup
Objective: Find the acceleration.
Approach: Draw free body diagrams for each mass individually.
Free Body Diagrams
Mass 1 (M1)
Forces acting on M1:
Normal force (N1) acting upwards.
Gravitational force (M1 * g) acting downwards.
Equation can be established:
In the Y direction: N1 = M1 * g (no vertical motion, hence the forces are balanced).
In the X direction:
Tension (T) acting to the right = M1 * a.
Mass 2 (M2)
Forces acting on M2:
Pull force (F0) acting to the right.
Tension (T) acting to the left.
Equation can be established:
In the X direction: F0 - T = M2 * a.
In the Y direction:
Normal force (N2) balances M2 * g downwards (forces balanced).
System Approach vs Individual Approach
Tension Calculation: Both equations have Tension (T) and acceleration (a) as unknowns, leading to complexity.
Alternatively, treat the two objects as a single system.
Center of Mass: Draw forces acting on the combined mass:
Normal force acts upwards.
Combined gravitational force down: (M1 + M2) * g.
F0 is the only external force acting in the horizontal direction.
Simplification through System Approach
For the system:
Y direction: N = (M1 + M2) * g (balances out).
X direction: F0 = (M1 + M2) * a.
Final equation for the system:
F0 = (M1 + M2) * a, where total mass is M1 + M2.
Tension becomes an internal force and cancels out when analyzing the system as one entity.
Atwood Machine Application
Setup: Atwood machine consists of a pulley system with two masses.
One known mass and an unknown mass to be determined using acceleration measurements.
Analyzing Motion in the Atwood Machine
Release system from rest; it will accelerate.
Connect the force interactions through free body diagrams for each mass:
Left mass (M1): Down: M1 * g, Up: Tension (T).
Equation if moving down: M1 * g - T = M1 * a.
Right mass (M2): Upwards: Tension (T), Down: M2 * g.
Equation: T - M2 * g = M2 * a.
Since tension is identical in a massless pulley system, consider behavior as a system for simplification.
Finding System Acceleration
External forces acting on the system:
M1 * g downward and M2 * g upward.
Total force: M1 * g - M2 * g = (M1 + M2) * a.
Solve for acceleration (a):
Use graphing techniques (velocity vs. time graph) to derive acceleration from slope.
Example of measured acceleration: a = 1.22 m/s².
Calculation of Unknown Mass
Substitute back into derived equations to solve:
Known mass (M2) = 0.05 kg.
Use: (M1 * g) - (M2 * g) = (M1 + M2) * 1.22 m/s².
After calculation: M1 ≈ 0.064 kg.
Comparison with real measured value: 0.065 kg.
Finding Tension in the String
After establishing acceleration and known masses, backtrack to find tension if needed:
Using the equation for the larger mass:
M1 * g - T = M1 * a.
Tension calculated ensuring all variables accounted.
Summary and Key Takeaways
System Approach: More efficient for solving acceleration.
Individual Force Analysis: Necessary for specific force calculations like tension.
Correct Methodology: Always write net force equations derived from free body diagrams to avoid skipping steps in calculations.